The Geometry of the CKM matrix, the Standard Model and RG fixed points
Brian P. Dolan, Charles Nash
Abstract
We investigate the geometry of the Fermion mixing matrix in the Standard Model. The principal structure studied is the CKM matrix, V, viewed as an element of the double coset space M, where M=T SU(3)/T, and T=U(1)× U(1). The space M is given a Riemannian metric, and has both point singularities, which it is shown correspond to the known renormalization group fixed points, and line singularities connecting the fixed points. A key discrete object inducing many of these properties is the Weyl group, W, of SU(3), W being the symmetric group S3, which appears in the guise of the vertices of a hexagon in V.
Create a lesson
Related papers
When duality changes the poles: SL(2,Z) transformations of linear response EFTs
Andrea Amoretti, Daniel K. Brattan, Jonas Rongen
Auxiliary Field Deformations of the Lambda Model
Christian Ferko, Cian Luke Martin, Pranat Sharma
Carrollian axion electrodynamics
Hemant Rathi, Ashish Shukla
The geometry of multiloop Feynman Integrals from the Scattering Facet
José Ríos-Sánchez, Germán Rodrigo
Deep learning emergent spacetime from fermionic spectral functions in holography
Koji Hashimoto, Hyun-Sik Jeong, Keun-Young Kim et al.
Schwinger stability of T-duality-inspired extremal black holes
Chiang-Mei Chen, Kimet Jusufi, Douglas Singleton